## Statistical Physics, Volume 5Elementary college physics course for students majoring in science and engineering. |

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Page 150

"I Measure level difference brought to this height

thermometer difference is kept

pressure gas ...

"I Measure level difference brought to this height

**Constant**-volume gasthermometer difference is kept

**constant**Measure-- height of mercury level**Constant**-pressure gas thermometer Fig. 4.4**Constant**-volume and**constant**-pressure gas ...

Page 279

S(TV) – S(To,Vo) = "coln # + R lin #| To Vo Or S(TV) = |coln T + R lin V +

(50) Adiabatic compression or expansion Consider an ideal gas which is

adiabatically isolated so that it cannot absorb any heat. Suppose now that the

volume ...

S(TV) – S(To,Vo) = "coln # + R lin #| To Vo Or S(TV) = |coln T + R lin V +

**constant**}(50) Adiabatic compression or expansion Consider an ideal gas which is

adiabatically isolated so that it cannot absorb any heat. Suppose now that the

volume ...

Page 292

/-Reservoir Z Temperature T Pressure p -—Piston Phase 2 >System Fig. 7.9 A

system which consists of two phases and which is maintained at a

temperature T and

reservoir.

/-Reservoir Z Temperature T Pressure p -—Piston Phase 2 >System Fig. 7.9 A

system which consists of two phases and which is maintained at a

**constant**temperature T and

**constant**pressure p by being kept in contact with a suitablereservoir.

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### Contents

Characteristic Features of Macroscopic Systems | 1 |

A I | 2 |

I | 6 |

Copyright | |

26 other sections not shown

### Common terms and phrases

absolute temperature absorbed accessible approximation assume atoms average Avogadro's calculate classical collision Consider constant container corresponding cules denote discussion distribution ensemble entropy equal equilibrium situation equipartition theorem example exchange energy expression external parameters fluctuations function given heat capacity heat Q heat reservoir Hence ideal gas initial internal energy interval isolated system kinetic energy large number left half liquid ln Q macroscopic parameters macroscopic system macrostate magnetic field magnetic moment magnitude mass mean energy mean number mean pressure mean value measured mechanics mole molecular momentum number of molecules occur oscillator particle particular partition phase space piston position possible values Prob quantity quantum numbers quasi-static random relation result simply solid specific heat spin system statistical statistical ensemble statistically independent Suppose thermal contact thermal interaction thermally insulated thermometer tion total energy total magnetic total number unit volume velocity